Prevailing Charge Order in Overdoped La_{2-x}Sr_{x}CuO_{4} beyond the Superconducting Dome.


Journal

Physical review letters
ISSN: 1079-7114
Titre abrégé: Phys Rev Lett
Pays: United States
ID NLM: 0401141

Informations de publication

Date de publication:
15 Sep 2023
Historique:
received: 30 09 2022
revised: 03 04 2023
accepted: 24 08 2023
medline: 29 9 2023
pubmed: 29 9 2023
entrez: 29 9 2023
Statut: ppublish

Résumé

The extremely overdoped cuprates are generally considered to be Fermi liquid metals without exotic orders, whereas the underdoped cuprates harbor intertwined states. Contrary to this conventional wisdom, using Cu L_{3}-edge and O K-edge resonant x-ray scattering, we reveal a charge order (CO) correlation in overdoped La_{2-x}Sr_{x}CuO_{4} (0.35≤x≤0.6) beyond the superconducting dome. This CO has a periodicity of ∼6 lattice units with correlation lengths of ∼20 lattice units. It shows similar in-plane momentum and polarization dependence and dispersive excitations as the CO of underdoped cuprates, but its maximum intensity differs along the c direction and persists up to 300 K. This CO correlation cannot be explained by the Fermi surface instability and its origin remains to be understood. Our results suggest that CO is prevailing in the overdoped metallic regime and requires a reassessment of the picture of overdoped cuprates as weakly correlated Fermi liquids.

Identifiants

pubmed: 37774302
doi: 10.1103/PhysRevLett.131.116002
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

116002

Auteurs

Qizhi Li (Q)

International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.

Hsiao-Yu Huang (HY)

National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan.

Tianshuang Ren (T)

Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou 310027, China.

Eugen Weschke (E)

Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin 14109, Germany.

Lele Ju (L)

Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou 310027, China.

Changwei Zou (C)

International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.

Shilong Zhang (S)

International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.

Qingzheng Qiu (Q)

International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.

Jiarui Liu (J)

Department of Physics and Astronomy, Clemson University, Clemson, South Carolina 29631, USA.

Shuhan Ding (S)

Department of Physics and Astronomy, Clemson University, Clemson, South Carolina 29631, USA.

Amol Singh (A)

National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan.

Oleksandr Prokhnenko (O)

Helmholtz-Zentrum Berlin für Materialien und Energie, Berlin 14109, Germany.

Di-Jing Huang (DJ)

National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan.

Ilya Esterlis (I)

Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA.

Yao Wang (Y)

Department of Physics and Astronomy, Clemson University, Clemson, South Carolina 29631, USA.
Department of Chemistry, Emory University, Atlanta, Georgia 30322, USA.

Yanwu Xie (Y)

Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics, Zhejiang University, Hangzhou 310027, China.

Yingying Peng (Y)

International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.
Collaborative Innovation Center of Quantum Matter, Beijing 100871, China.

Classifications MeSH